I shall first address the early discovery of unconventional superconductivity in the heavy-fermion (HF) metal CeCu2Si2. Then two fundamentally different antiferromagnetic quantum-critical-point (QCP) scenarios proposed for HF metals will be briefly discussed. CeCu2Si2 turns out to be the prototype of a conventional quantum critical material. Here, a three-dimensional spin-density-wave (SDW) QCP exists, and almost quantum-critical spin fluctuations are driving the formation of Cooper pairs.
An unconventional antiferromagnetic QCP, frequently called a 4f-orbital-selective Mott transition, at which the Kondo effect becomes destroyed, has been identified in a small number of HF systems, e.g., CeCu6-xAux [7] and YbRh2Si2. In both compounds, no superconductivity exists at T > 10 mK. However, HF superconductivity with maximum Tc ≈ 2.3 K develops in the vicinity of the pressure-induced Kondo-destroying QCP (pc ≈ 2.3 GPa) for CeRhIn5. Future research activities will have to unravel the potential differences between HFSC, driven by SDW fluctuations, and HFSC that forms in the vicinity of an orbital-selective Mott transition.
个人简介:
Frank Steglich discovered the first heavy fermion superconductor, CeCu 2Si 2, while working as a postdoctoral student in Cologne, Germany in 1978. CeCu 2Si 2 is the first metallic system to be discovered in which the superconductivity is driven by electron-electron interactions, rather than the electron-phonon interaction that is responsible for conventional BCS superconductivity. The discovery of this material revolutionized research into superconductivity, establishing the reality of electronically mediated superconductivity and foreshadowing the discovery of a wide range of heavy electron superconductors, and the subsequent discovery of electronically mediated pairing in cuprate high temperature superconductors. The first published report of the phenomenon occurred in 1979, by which time Steglich had taken up a junior faculty position at the University of Darmstadt, and confirmed the existence of bulk superconductivity through the measurement of the specific heat anomaly at the transition temperature of T c=0.5K. |